𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Edge Plasma Transport in the Helical Divertor Configuration in LHD

✍ Scribed by S. Masuzaki; M. Kobayashi; T. Murase; T. Morisaki; M. Tokitani; N. Ohyabu; H. Yamada; A. Komori; LHD Experiment Group

Publisher
John Wiley and Sons
Year
2010
Tongue
English
Volume
50
Category
Article
ISSN
0005-8025

No coin nor oath required. For personal study only.

πŸ“œ SIMILAR VOLUMES

3D Divertor Transport Study of the Local
3D Divertor Transport Study of the Local Island Divertor Configuration in the Large Helical Device
✍ M. Kobayashi; Y. Feng; D. Reiter; T. Morisaki; S. Masuzaki; F. Sardei; N. Ohyabu πŸ“‚ Article πŸ“… 2006 πŸ› John Wiley and Sons 🌐 English βš– 949 KB

The divertor/SOL transport of the Local Island Divertor (LID) configuration in the Large Helical Device (LHD) is studied. Since the LID configuration has an inherent three dimensional magnetic structure, the 3D edge transport code, EMC3-EIRENE, is applied in order to elucidate the 3D divertor transp

Optimization of Closed Divertor Configur
Optimization of Closed Divertor Configuration for Effective Particle Control in LHD Plasmas
✍ M. Shoji; M. Kobayashi; S. Masuzaki; T. Watanabe; A. Iwamae; H. Yamada; A. Komor πŸ“‚ Article πŸ“… 2008 πŸ› John Wiley and Sons 🌐 English βš– 179 KB

## Abstract Neutral particles in the LHD plasma periphery are investigated by three‐dimensional neutral particle transport simulation. The simulation predicts significant change of the density profile of neutral particles depending on magnetic configurations (radial position of the magnetic axis R~

Effect of Magnetic Ergodicity on Edge Pl
Effect of Magnetic Ergodicity on Edge Plasma Structure and Divertor Flux Distribution in LHD
✍ T. Morisaki; S. Masuzaki; M. Goto; S. Morta; A. Komori; N. Ohyabu; O. Motojima; πŸ“‚ Article πŸ“… 2002 πŸ› John Wiley and Sons 🌐 English βš– 404 KB πŸ‘ 2 views

Strong nonuniformity in the helical divertor flux distribution is seen both in numerical calculations and in experiments. Flux profiles along the divertor trace on the vacuum vessel change according to vacuum magnetic configurations. Diverted particles choose one of two X-points as the escaping chan